We also define the transmission rate space as.
Let denote the transmission rate space of each channel, in which is corresponding to -QAM transmission.
The rate space K:=[c,B] I J N is clearly compact, since R i j b ∈[c,B],B<∞,c>0.
Second, the monotonic structure of the rate space problem is exploited to compute a globally optimal rate vector with an outer approximation algorithm.
In the strain rate space, the computational quintiple-solution multiplicity extends from ∼ 100 10,000 s−1, at 9% H2 in N2 and 4 atm.
The effect of glycerin to water ratio, metal loading, and the feed flow rate (space velocity) was analyzed for the two best performing catalysts.
These compression studies confirmed that deformation in the temperature-strain rate space evaluated is matrix-controlled, yielding an activation energy of ∼415 445 kJ/mol.
We argue that these can be used to cover a wide region of the nucleation rate space, hence facilitating comparison with experiments.
Equipotential surfaces in strain rate space and corresponding yield loci obtained by the new method for four materials (one ferrite single crystal, one aluminium alloy and two types of steel) are presented and discussed.
In particular, the solution proposed in [15] is tailored for the rate space-time block code introduced by Tarokh in [16] and assumes a static channel with a single DOA for each user.
Since the code rate space is { 4 / 4, 4 / 5, 4 / 6, …, 4 / 12 }, which contains nine possible values, instead of multiplying w, a random integer, rand ∼ Rand 0,w), could be applied as r i right = r i + rand in simulation.
